A self-consistent interactive model for the study of luminescence coupling in multijunction solar cells

2021 ◽  
Vol 130 (24) ◽  
pp. 243103
Author(s):  
Daniel N. Micha ◽  
Ricardo T. Silvares
2013 ◽  
Vol 103 (26) ◽  
pp. 263907 ◽  
Author(s):  
Tomah Sogabe ◽  
Akio Ogura ◽  
Chao-Yu Hung ◽  
Valery Evstropov ◽  
Mikhail Mintairov ◽  
...  

2020 ◽  
Vol 28 (11) ◽  
pp. 1097-1106
Author(s):  
Iván Lombardero ◽  
Mario Ochoa ◽  
Naoya Miyashita ◽  
Yoshitaka Okada ◽  
Carlos Algora

2005 ◽  
Vol 40 (10-11) ◽  
pp. 1039-1042 ◽  
Author(s):  
G. Timò ◽  
C. Flores ◽  
R. Campesato

Author(s):  
Guillaume Courtois ◽  
Rufi Kurstjens ◽  
Jinyoun Cho ◽  
Kristof Dessein ◽  
Ivan Garcia ◽  
...  

Coatings ◽  
2021 ◽  
Vol 11 (4) ◽  
pp. 398
Author(s):  
Pablo Caño ◽  
Carmen M. Ruiz ◽  
Amalia Navarro ◽  
Beatriz Galiana ◽  
Iván García ◽  
...  

Gallium phosphide (GaP) is an ideal candidate to implement a III-V nucleation layer on a silicon substrate. The optimization of this nucleation has been pursued for decades, since it can form a virtual substrate to grow monolithically III-V devices. In this work we present a GaP nucleation approach using a standard MOVPE reactor with regular precursors. This design simplifies the epitaxial growth in comparison to other routines reported, making the manufacturing process converge to an industrial scale. In short, our approach intends to mimic what is done to grow multijunction solar cells on Ge by MOVPE, namely, to develop a growth process that uses a single reactor to manufacture the complete III-V structure, at common MOVPE process temperatures, using conventional precursors. Here, we present the different steps in such GaP nucleation routine, which include the substrate preparation, the nucleation itself and the creation of a p-n junction for a Si bottom cell. The morphological and structural measurements have been made with AFM, SEM, TEM and Raman spectroscopy. These results show a promising surface for subsequent III-V growth with limited roughness and high crystallographic quality. For its part, the electrical characterization reveals that the routine has also formed a p-n junction that can serve as bottom subcell for the multijunction solar cell.


2019 ◽  
Vol 28 (1) ◽  
pp. 16-24 ◽  
Author(s):  
Kikuo Makita ◽  
Hidenori Mizuno ◽  
Takeshi Tayagaki ◽  
Taketo Aihara ◽  
Ryuji Oshima ◽  
...  

2011 ◽  
Vol 50 (9) ◽  
pp. 092302 ◽  
Author(s):  
Gia-Wei Shu ◽  
Chiun-Hsiang Tung ◽  
Shr-Chang Tung ◽  
Po-Chen Su ◽  
Ji-Lin Shen ◽  
...  

1985 ◽  
Author(s):  
James A. Hutchby ◽  
Robert J. Markunas ◽  
Salah M. Bedair

2010 ◽  
Vol 74 ◽  
pp. 225-230 ◽  
Author(s):  
Vladimir M. Lantratov ◽  
Viktor M. Emelyanov ◽  
Nikolay A. Kalyuzhnyy ◽  
Sergey A. Mintairov ◽  
Maxim Z. Shvarts

Feasibility to increase the radiation resistance of multijunction solar cells in using Bragg reflectors has been shown. Two designs of Bragg reflectors for multijunction solar cells, which allow ensuring in the Ga(In)As subcell base an effective collection of minority charge carriers at the decrease of their diffusion length caused by radiation treatment, have been investigated. Influence of subcells’ thicknesses of n-p GaInP/Ga(In)As/Ge solar cell under 1 MeV electron irradiation with fluences up to 3•1015 cm–2 on short circuit current was considered. Optimal thicknesses of GaInP and GaInAs subcells with Bragg reflectors, depending on the rated operation period on the geostationary orbit, were estimated. It has been shown that such an optimization allows to achieve efficiency at long operation of solar cells on the orbit noticeably higher than that of non-optimized cells.


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